\rule{\textwidth}{0.1mm}
$$ \bl{\large \textbf{Transformările simple ale gazului ideal}} $$
$$ \gr{\Delta U = Q - L} $$
{\fontsize{8pt}{8pt} \selectfont
$$ nln
\begin{array}{|c||c|c|c|c|c|}
\hline
& & & & & \\
\gr{\text{Transformarea}} & \gr{\text{Definiţie}} & \gr{\text{Lege}} & \gr{\Delta U} & \gr{Q} & \gr{L}\\
& & & & & \\
\hline\hline
& & & & & \\
\text{izocoră} & V_1=V_2 & \dfrac{p_1}{T_1}=\dfrac{p_2}{T_2} & \nu C_V\Delta T=\dfrac{C_V}{R}V\Delta p & \nu C_V\Delta T=\dfrac{C_V}{R}V\Delta p & 0\\
& & & & & \\
\text{izobară} & p_1=p_2 & \dfrac{V_1}{T_1}=\dfrac{V_2}{T_2} & \nu C_V\Delta T=\dfrac{C_V}{R}p\Delta V & \nu C_p \Delta T=\dfrac{C_p}{R}p\Delta V nln
& \nu R\Delta T=p\Delta V\\
& & & & & \\
\text{izotermă} & T_1=T_2 & p_1V_1=p_2V_2 & 0 & \nu RT\ln\dfrac{V_2}{V_1} & \nu RT\ln\dfrac{V_2}{V_1}\\
& & & & & \\
\text{adiabatică} & Q=0 & p_1V_1^{\gamma}=p_2V_2^{\gamma} & \nu C_V\Delta T=\dfrac{C_V}{R}\Delta (pV) & 0 & nln
-\nu C_V\Delta T=-\dfrac{C_V}{R}\Delta (pV)\\
& & & & & \\
\hline
\end{array} nln
$$ }
$$ \nu=\dfrac{N}{N_A}=\dfrac{m}{\mu}\qquad pV = \nu RT\qquad C_V = \dfrac{i}{2}R\qquad C_p = C_V + R\qquad \gamma = \dfrac{C_p}{C_V}$$